The diffusivity of Mg in monocrystalline Co1-xO samples was studied, at temperatures ranging from 1000 to 1600C and O partial pressures ranging from 10-8 to 0.21atm, by using microprobe analysis and secondary ion mass spectrometry methods. It was found that the results (table 60) could be described by the expression:
D (cm2/s) = 0.014 exp[-1.95(eV)/kT]
for an O partial pressure of 0.21atm and temperatures of between 1000 and 1600C, and by the expression:
D (cm2/s) = 0.004 exp[-2.07(eV)/kT]
for an O partial pressure of 10-5atm, and temperatures of between 1060 and 1455C. The dependence of the diffusivity upon the O partial pressure was of the form:
log [D (cm2/s)] = 0.0035[log(PO2)]2 + 0.22 log(PO2) - 8.4
at a temperature of 1200C and for pressures of between 10-8 and 0.21atm. It was concluded that the effect of the partial pressure upon Mg impurity diffusion was greater than that upon Co self-diffusion. This was attributed to a preferential attractive interaction
between VCo" and Mg.
H.Boussetta, C.Monty: Journal of the Physics and Chemistry of Solids, 1988, 49[4], 369-75
Table 59
Diffusion Parameters for Ga in (Co1-xGax)O at 1100 to 1350C
log [O2 activity] | x (at%) | Do (cm2/s) | E (kJ/mol) |
-0.67 | 0.00 | 0.00032 | 123 |
-0.67 | 0.32 | 0.00034 | 123 |
-0.67 | 0.79 | 0.00056 | 129 |
-0.67 | 1.64 | 0.0041 | 152 |
-3.20 | 0.00 | 0.00020 | 135 |
-3.20 | 0.32 | 0.00029 | 132 |
-3.20 | 0.79 | 0.00058 | 136 |
-3.20 | 1.64 | 0.0030 | 154 |
-7.00 | 0.00 | 0.020 | 204 |
-7.00 | 0.32 | 0.00013 | 157 |
-7.00 | 0.79 | 0.000089 | 120 |